Camera Optical Lens

ABSTRACT

The present disclosure discloses a camera optical lens. The camera optical lens including, in an order from an object side to an image side, a first lens having a positive refractive power, a second lens having a negative refractive power, a third lens having a positive refractive power, a fourth lens having a negative refractive power, a fifth lens having a positive refractive power, and a sixth lens having a negative refractive power. The camera optical lens further satisfies specific conditions.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims the priority benefit of Japanese Patent Applications Ser. No. 2018-041754 filed on Mar. 8, 2018, the entire content of which is incorporated herein by reference.

FIELD OF THE PRESENT DISCLOSURE

The present disclosure relates to optical lens, in particular to a camera optical lens suitable for handheld devices such as smart phones and digital cameras and imaging devices.

Description of Related Art

In recent years, the demand for miniature camera lens is increasing day by day, but the photosensitive devices of general camera lens are no other than Charge Coupled Device (CCD) or Complementary metal-Oxide Semiconductor Sensor (CMOS sensor), and as the progress of the semiconductor manufacturing technology makes the pixel size of the photosensitive devices shrink, coupled with the current development trend of electronic products being that it should have excellent optical characteristics and high light flux and their shape should be small, miniature camera lens with good imaging quality therefor has become a mainstream in the market.

A typical related camera lens comprises six lenses, and from the object side to the image side, the camera lens comprises in sequence: a first lens having a positive refractive power, a second lens having a negative refractive power, a third lens having a positive refractive power, a fourth lens having a negative refractive power, a fifth lens having a positive refractive power, and a sixth lens having a negative refractive power.

However, the refractive index distribution of the first lens and the shape of the first lens and the fourth lens are insufficient, the luminance is not sufficient for Fno≥2.14. In other traditional camera lenses, although Fno≥2.15, but the luminance is also insufficient.

BRIEF DESCRIPTION OF THE DRAWINGS

Many aspects of the exemplary embodiments can be better understood with reference to the following drawings. The components in the drawing are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the present disclosure.

FIG. 1 is a schematic diagram of a camera optical lens LA in accordance with an embodiment of the present invention;

FIG. 2 is a schematic diagram of a camera optical lens in accordance with a first embodiment of the present invention;

FIG. 3 shows the longitudinal aberration of the camera optical lens shown in FIG. 2;

FIG. 4 shows the lateral color of the camera optical lens shown in FIG. 2;

FIG. 5 presents a schematic diagram of the field curvature and distortion of the camera optical lens shown in FIG. 2;

FIG. 6 is a schematic diagram of a camera optical lens in accordance with a second embodiment of the present invention;

FIG. 7 presents the longitudinal aberration of the camera optical lens shown in FIG. 6;

FIG. 8 presents the lateral color of the camera optical lens shown in FIG. 6;

FIG. 9 presents the field curvature and distortion of the camera optical lens shown in FIG. 6;

FIG. 10 is a schematic diagram of a camera optical lens in accordance with a third embodiment of the present invention;

FIG. 11 presents the longitudinal aberration of the camera optical lens shown in FIG. 10;

FIG. 12 presents the lateral color of the camera optical lens shown in FIG. 10;

FIG. 13 presents the field curvature and distortion of the camera optical lens shown in FIG. 10.

DETAILED DESCRIPTION OF THE EXEMPLARY EMBODIMENTS

The present disclosure will hereinafter be described in detail with reference to several exemplary embodiments. To make the technical problems to be solved, technical solutions and beneficial effects of the present disclosure more apparent, the present disclosure is described in further detail together with the figure and the embodiments. It should be understood the specific embodiments described hereby is only to explain the disclosure, not intended to limit the disclosure.

As referring to FIG. 1, the present invention provides a camera lens LA. FIG. 1 shows a schematic diagram of a camera lens LA in accordance with an embodiment of the present invention. The camera optical lens LA comprises 6 lenses. Specifically, from the object side to the image side, the camera optical lens LA comprises in sequence: a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, and a sixth lens L6. A glass panel GF can be arranged between the sixth lens L6 and the image surface. The glass plate GF can be a cover-glass or a filter with IR cut-off function. In another embodiment, the camera lens could also be configured to including the six lens L6 and the image plane without the glass panel GF.

The first lens L1 has a positive refractive power, the second lens L2 has a negative refractive power, the third lens L3 has a positive refractive power, the fourth lens L4 has a negative refractive power, the fifth lens L5 has a positive refractive power, and the sixth lens L6 has a negative refractive power. In order to correct the aberration problem, the surface of the six lens should be designed to aspherical surface.

Here, the focal length of the whole camera optical lens LA is defined as f, the focal length of the first lens is defined as f1. The camera optical lens LA further satisfies the following condition: 1.00≤f1/f≤1.10 Condition 1.00≤f1/f≤1.10 fixes the positive refractive power of the first lens L1. If the lower limit of the set value is exceeded, although it benefits the ultra-thin development of lenses, but the positive refractive power of the first lens L1 will be too strong, problem like aberration is difficult to be corrected. On the contrary, if the upper limit of the set value is exceeded, the positive refractive power of the first lens L1 becomes too weak, it is then difficult to develop miniaturized lenses.

The curvature radius of the object side surface of the first lens L1 is defined as R1, the curvature radius of the image side surface of the first lens L1 is defined as R2. The following condition should be satisfied: −2.40≤(R1+R2)/(R1−R2)≤−1.90, by which, the shape of the first lens L1 is fixed, further, and when beyond this range, it is unfavorable for realization of high light flux (Fno), excellent optical characteristics and miniaturization.

The curvature radius of the object side surface of the fourth lens L4 is defined as R7, the curvature radius of the image side surface of the fourth lens L4 is defined as R8. The following condition should be satisfied: 11.40≤(R7+R8)/(R7−R8)≤16.00, by which, the shape of the fourth lens L4 is fixed, further, when beyond this range, it is unfavorable for realization of high light flux (Fno), excellent optical characteristics and miniaturization.

The second lens L2 has a negative refractive power and the fourth lens L4 has a negative refractive power. The focal length of the second lens L2 is f2, the focal length of the fourth lens L4 is f4. The following condition should be satisfied: 0.15≤f2/f4≤0.16. This condition fixes the ratio between the focal length of the second lens L2 and the focal length of the fourth lens L4. When beyond this range, it is unfavorable for realization of high light flux (Fno), excellent optical characteristics and miniaturization.

The sixth lens L6 has a negative refractive power. The focal length of the whole camera optical lens LA is f, the curvature radius of the object side surface of the sixth lens L6 is defined as R11. The following condition should be satisfied: 2.30≤R11/f≤2.50. This condition fixes the ratio between the curvature radius of the object side surface of the sixth lens L6 and the focal length of the whole camera optical lens LA. When beyond this range, it is unfavorable for realization of high light flux (Fno), excellent optical characteristics and miniaturization.

When the focal length of the camera optical lens LA of the present invention, the focal length of each lens, the refractive power of the related lens, and the curvature radius of the camera optical lens satisfy the above conditions, the camera optical lens LA has the advantage of high light flux (Fno), excellent optical characteristics and miniaturization.

In the following, an example will be used to describe the camera optical lens LA of the present invention. The symbols recorded in each example are as follows. The unit of distance, radius and center thickness is mm

f: The focal length of the camera lens;

f1: The focal length of the first lens;

f2: The focal length of the second lens;

f3: The focal length of the third lens;

f4: The focal length of the fourth lens;

f5: The focal length of the fifth lens;

f6: The focal length of the sixth lens;

Fno: F value;

2ω: Field;

S1: Aperture;

R: The curvature radius of the optical surface, the central curvature radius in case of lens;

R1: The curvature radius of the object side surface of the first lens L1;

R2: The curvature radius of the image side surface of the first lens L1;

R3: The curvature radius of the object side surface of the second lens L2;

R4: The curvature radius of the image side surface of the second lens L2;

R5: The curvature radius of the object side surface of the third lens L3;

R6: The curvature radius of the image side surface of the third lens L3;

R7: The curvature radius of the object side surface of the fourth lens L4;

R8: The curvature radius of the image side surface of the fourth lens L4;

R9: The curvature radius of the object side surface of the fifth lens L5;

R10: The curvature radius of the image side surface of the fifth lens L5;

R11: The curvature radius of the object side surface of the sixth lens L6;

R12: The curvature radius of the image side surface of the sixth lens L6;

R13: The curvature radius of the object side surface of the optical filter GF;

R14: The curvature radius of the image side surface of the optical filter GF;

d: The thickness on-axis of the lens and the distance on-axis between the lens;

d0: The distance on-axis from aperture S1 to the object side surface of the first lens L1;

d1: The thickness on-axis of the first lens L1;

d2: The distance on-axis from the image side surface of the first lens L1 to the object side surface of the second lens L2;

d3: The thickness on-axis of the second lens L2;

d4: The distance on-axis from the image side surface of the second lens L2 to the object side surface of the third lens L3;

d5: The thickness on-axis of the third lens L3;

d6: The distance on-axis from the image side surface of the third lens L3 to the object side surface of the fourth lens L4;

d7: The thickness on-axis of the fourth lens L4;

d8: The distance on-axis from the image side surface of the fourth lens L4 to the object side surface of the fifth lens L5;

d9: The thickness on-axis of the fifth lens L5;

d10: The distance on-axis from the image side surface of the fifth lens L5 to the object side surface of the sixth lens L6;

d11: The thickness on-axis of the sixth lens L6;

d12: The distance on-axis from the image side surface of the sixth lens L6 to the object side surface of the optical filter GF;

d13: The thickness on-axis of the optical filter GF;

d14: The distance on-axis from the image side surface to the image surface of the optical filter GF;

nd: The refractive power of the d line;

nd1: The refractive power of the d line of the first lens L1;

nd2: The refractive power of the d line of the second lens L2;

nd3: The refractive power of the d line of the third lens L3;

nd4: The refractive power of the d line of the fourth lens L4;

nd5: The refractive power of the d line of the fifth lens L5;

nd6: The refractive power of the d line of the sixth lens L6;

nd7: The refractive power of the d line of the optical filter GF;

vd: The abbe number;

v1: The abbe number of the first lens L1;

v2: The abbe number of the second lens L2;

v3: The abbe number of the third lens L3;

v4: The abbe number of the fourth lens L4;

v5: The abbe number of the fifth lens L5;

v6: The abbe number of the sixth lens L6;

v7: The abbe number of the optical filter GF.

IH: Image height;

TTL: Optical length (the distance on-axis from the object side surface of the first lens L1 to the image surface);

LB: The distance on-axis from the image side surface of the sixth lens L6 to the image surface (including the thickness of the glass plate GF);

y=(x ² /R)/[1+{1−(k+1)(x ² /R2)}^(1/2) ]+A4x ⁴ +A6x ⁶ +A8x ⁸ +A10x ¹⁰ +A12x ¹² +A14x ¹⁴ +A16x ¹⁶ +A18x ¹⁸ +A20x ²⁰   (1)

Among them, K is a conic index, A4, A6, A8, A10, A12, A14, A16 A18, A20 are aspheric surface indexes.

For convenience, the aspheric surface of each lens surface uses the aspheric surfaces shown in the above condition (1). However, the present invention is not limited to the aspherical polynomials form shown in the condition (1).

Embodiment 1

FIG. 2 is a schematic diagram of the camera lens LA in accordance with a first embodiment of the present invention. The data of table 1 includes: the curvature radius R of the object side and the image side from the first lens L1 to the sixth lens L6

the central distance of lens and the distance d between lenses

the refractive power nd and the abbe number vd. The data of table 2 includes: conic index k

aspheric surface index.

TABLE 1 R d nd v d S1 ∞ d0 = −0.400 R1 1.65682 d1 = 0.598 nd1 1.5441 v 1 56.04 R2 4.44584 d2 = 0.056 R3 4.27155 d3 = 0.233 nd2 1.6614 v 2 20.41 R4 2.36212 d4 = 0.257 R5 2.92027 d5 = 0.441 nd3 1.5441 v 3 56.04 R6 7.14159 d6 = 0.448 R7 5.75237 d7 = 0.325 nd4 1.6398 v 4 23.27 R8 4.83575 d8 = 0.393 R9 6.19213 d9 = 0.564 nd5 1.5441 v 5 56.04 R10 −4.28608 d10 = 0.243 R11 10.14013 d11 = 0.343 nd6 1.5441 v 6 56.04 R12 1.41653 d12 = 0.350 R13 ∞ d13 = 0.300 ndg 1.5168 vg 64.17 R14 ∞ d14 = 0.392

Table 2 shows the aspherical surface data of the camera optical lens LA in the embodiment 1 of the present invention.

TABLE 2 Conic Index Aspherical Surface Index k A4 A6 A8 A10 R1 −7.3096E−05 −7.7522E−03 2.7173E−02 −7.7363E−02 9.4978E−02 R2 −5.0661E−03 −1.1602E−01 2.7521E−01 −4.0231E−01 2.9096E−01 R3 6.9197E−03 −1.7435E−01 4.2348E−01 −5.5670E−01 3.9319E−01 R4 −2.5853E−0.3 −1.2075E−01 3.2303E−01 −4.5563E−01 4.4034E−01 R5 2.2078E−03 −6.4554E−02 3.9610E−02 3.2971E−02 −2.8316E−01 R6 7.5761E−02 −5.5738E−02 2.6956E−03 8.4503E−02 −3.2345E−01 R7 4.6944E−02 −1.4435E−01 1.0530E−02 1.5580E−01 −3.5343E−01 R8 −1.3192E−02 −1.6949E−01 7.7943E−02 −3.9263E−02 1.1546E−02 R9 7.7019E−02 −7.4645E−03 −4.2344E−02 −9.4285E−03 2.6541E−02 R10 −4.4669E+01 5.4031E−02 −4.3121E−02 2.6460E−02 −2.1739E−02 R11 1.1120E−01 −3.0539E−01 1.9838E−01 −7.7608E−02 2.1680E−02 R12 −8.1878E+00 −1.4997E−01 8.4696E−02 −3.3079E−02 7.5243E−03 Aspherical Surface Index A12 A14 A16 A18 A20 R1 −6.6391E−02 1.9259E−02 −2.2869E−03 — — R2 −9.5822E−02 4.3789E−03 2.4737E−03 — — R3 −9.9777E−02 −1.2918E−02 6.5498E−03 — — R4 −2.5242E−01 1.1049E−01 −2.9670E−02 — — R5 4.5553E−01 −3.2601E−01 9.1477E−02 — — R6 4.1873E−01 −2.6132E−01 6.4820E−02 — — R7 3.3416E−01 −1.6446E−01 3.2921E−02 — — R8 −7.8459E−03 5.9477E−03 −1.2200E−03 — — R9 −2.2889E−02 6.6625E−03 4.3017E−04 −3.9591E−04 3.2912E−05 R10 1.0859E−02 −3.0670E−03 5.1467E−04 −4.9432E−05 2.1071E−06 R11 −4.5053E−03 7.1938E−04 −8.7641E−05 7.1646E−06 −2.7854E−07 R12 −7.9053E−04 −1.7760E−05 1.3218E−05 −1.2153E−06 3.6877E−08

Table 7 shows the various values of the embodiments 1, 2, 3, and the values corresponding with the parameters which are already specified in the conditions.

As shown in Table 7, the first embodiment satisfies the various conditions.

FIG. 3 and FIG. 4 show the longitudinal aberration and lateral color schematic diagrams after light with a wavelength of 486 nm, 588 nm and 656 nm passes the camera optical lens LA in the first embodiment. FIG. 5 shows the field curvature and distortion schematic diagrams after light with a wavelength of 588 nm passes the camera optical lens LA in the first embodiment, the field curvature S in FIG. 5 is a field curvature in the sagittal direction, T is a field curvature in the meridian direction. This is the same as in embodiment 2 and embodiment 3. As shown in FIG. 3 to FIG. 5, in this embodiment, the optical length TTL of the camera optical lens is 4.942 mm, the F value Fno is 1.82, it has an excellent optical characteristics with miniaturization and high light flux (Fno).

Embodiment 2

FIG. 6 is a schematic diagram of the camera lens LA in accordance with a second embodiment of the present invention. The data of table 1 includes: the curvature radius R of the object side and the image side from the first lens L1 to the sixth lens L6

the central distance of lens and the distance d between lenses

the refractive power nd and the abbe number vd. The data of table 2 includes: conic index k

aspheric surface index.

Table 3 and table 4 show the design data of the camera optical lens 20 in embodiment 2 of the present invention.

TABLE 3 R d nd νd S1 ∞ d0 = −0.400 R1 1.68662 d1 = 0.562 nd1 1.5441 ν1 56.04 R2 5.00226 d2 = 0.046 R3 4.32430 d3 = 0.226 nd2 1.6614 ν2 20.41 R4 2.53903 d4 = 0.279 R5 3.06567 d5 = 0.393 nd3 1.5441 ν3 56.04 R6 6.68294 d6 = 0.458 R7 5.41132 d7 = 0.293 nd4 1.6398 ν4 23.27 R8 4.67508 d8 = 0.356 R9 6.75979 d9 = 0.589 nd5 1.5441 ν5 56.04 R10 −4.50657 d10 = 0.230 R11 10.02818 d11 = 0.411 nd6 1.5441 ν6 56.04 R12 1.42731 d12 = 0.350 R13 ∞ d13 = 0.300 nd7 1.5168 ν7 64.17 R14 ∞ d14 = 0.377

Table 4 shows the aspherical surface data of each lens of the camera optical lens 20 in embodiment 2 of the present invention.

TABLE 4 Conic Index Aspherical Surface Index k A4 A6 A8 A10 R1 −1.8622E−02 −8.9916E−03 2.6716E−02 −7.7670E−02 9.4983E−02 R2 −1.5152E+00 −1.1791E−01 2.7331E−01 −4.0282E−01 2.9148E−01 R3 −1.8770E+00 −1.7760E−01 4.2258E−01 −5.5801E−01 3.9130E−01 R4 1.8088E−01 −1.1748E−01 3.1930E−01 −4.6111E−01 4.3581E−01 R5 2.2705E−01 −6.3146E−02 3.8893E−02 3.5544E−02 −2.8003E−01 R6 −1.3068E+01 −5.9907E−02 7.2847E−03 8.6036E−02 −3.2413E−01 R7 4.7347E−01 −1.4389E−01 7.5080E−03 1.5522E−01 −3.5328E−01 R8 1.4876E+00 −1.6692E−01 7.6734E−02 −4.0102E−02 1.1374E−02 R9 2.6135E+00 −3.7496E−03 −4.4209E−02 −9.6328E−03 2.6575E−02 R10 −3.5687E+01 5.6222E−02 −4.3414E−02 2.6362E−02 −2.1754E−02 R11 −3.1194E+00 −3.0593E−01 1.9828E−01 −7.7618E−02 2.1679E−02 R12 −7.6463E+00 −1.4911E−01 8.4572E−02 −3.3102E−02 7.5207E−03 Aspherical Surface Index A12 A14 A16 A18 A20 R1 −6.6268E−02 1.9326E−02 −2.3477E−03 — — R2 −9.4978E−02 4.6819E−03 2.0220E−03 — — R3 −1.0142E−01 −1.3468E−02 7.5070E−03 — — R4 −2.5493E−01 1.0989E−01 −2.8935E−02 — — R5 4.5703E−01 −3.2642E−01 8.9860E−02 — — R6 4.1813E−01 −2.6110E−01 6.5698E−02 — — R7 3.3406E−01 −1.6506E−01 3.1936E−02 — — R8 −7.7899E−03 6.0219E−03 −1.1745E−03 — — R9 −2.2870E−02 6.6676E−03 4.3161E−04 −3.9526E−04 3.3278E−05 R10 1.0857E−02 −3.0672E−03 5.1465E−04 −4.9438E−05 2.1043E−06 R11 −4.5053E−03 7.1941E−04 −8.7632E−05 7.1665E−06 −2.7824E−07 R12 −7.9087E−04 −1.7774E−05 1.3221E−05 −1.2144E−06 3.7065E−08

As shown in Table 7, the second embodiment satisfies the various conditions.

FIG. 7 and FIG. 8 show the longitudinal aberration and lateral color schematic diagrams after light with a wavelength of 486 nm, 588 nm and 656 nm passes the camera optical lens 20 in the second embodiment. FIG. 9 shows the field curvature and distortion schematic diagrams after light with a wavelength of 588 nm passes the camera optical lens in the second embodiment. As shown in FIG. 7 to FIG. 9, in this embodiment, the optical length TTL of the camera optical lens is 4.870 mm, the F value Fno is 1.82, it has an excellent optical characteristics with miniaturization and high light flux (Fno).

Embodiment 3

FIG. 10 is a schematic diagram of the camera lens LA in accordance with embodiment 3 of the present invention. The data of table 1 includes: the curvature radius R of the object side and the image side from the first lens L1 to the sixth lens L6

the central distance of lens and the distance d between lenses

the refractive power nd and the abbe number vd. The data of table 2 includes: conic index k

aspheric surface index.

Table 5 and table 6 show the design data of the camera optical lens 30 in embodiment 3 of the present invention.

TABLE 5 R d nd νd S1 ∞ d0 = −0.400 R1 1.63757 d1 = 0.595 nd1 1.5441 ν1 56.04 R2 4.15668 d2 = 0.039 R3 4.38406 d3 = 0.235 nd2 1.6614 ν2 20.41 R4 2.55654 d4 = 0.282 R5 3.07508 d5 = 0.441 nd3 1.5441 ν3 56.04 R6 7.27057 d6 = 0.464 R7 4.15958 d7 = 0.287 nd4 1.6398 ν4 23.27 R8 3.66436 d8 = 0.386 R9 6.83702 d9 = 0.566 nd5 1.5441 ν5 56.04 R10 −4.28035 d10 = 0.226 R11 10.44120 d11 = 0.367 nd6 1.5441 ν6 56.04 R12 1.42705 d12 = 0.350 R13 ∞ d13 = 0.300 ndg 1.5168 νg 64.17 R14 ∞ d14 = 0.387

Table 6 shows the aspherical surface data of each lens of the camera optical lens 30 in embodiment 3 of the present invention.

TABLE 6 Conic Index Aspherical Surface Index k A4 A6 A8 A10 R1 7.0126E−03 −8.1439E−03 2.8159E−02 −7.6472E−02 9.5502E−02 R2 −7.4194E−01 −1.1728E−01 2.7345E−01 −4.0284E−01 2.9129E−01 R3 −1.1608E+00 −1.7661E−01 4.2346E−01 −5.5706E−01 3.9241E−01 R4 4.0591E−01 −1.1549E−01 3.2312E−01 −4.5718E−01 4.3911E−01 R5 1.9904E−02 −6.4129E−02 3.6747E−02 3.3107E−02 −2.8092E−01 R6 −1.0425E+01 −5.9844E−02 4.5817E−03 8.6609E−02 −3.2240E−01 R7 −1.6736E+00 −1.4568E−01 1.0422E−02 1.5670E−01 −3.5272E−01 R8 −1.1760E−01 −1.6957E−01 7.7561E−02 −3.9747E−02 1.1292E−02 R9 6.7504E+00 −2.9036E−03 −4.4045E−02 −9.7755E−03 2.6520E−02 R10 −4.2834E+01 5.4355E−02 −4.3147E−02 2.6446E−02 −2.1743E−02 R11 4.8860E−02 −3.0539E−01 1.9837E−01 −7.7611E−02 2.1679E−02 R12 −8.3977E+00 −1.5011E−01 8.4680E−02 −3.3087E−02 7.5230E−03 Aspherical Surface Index A12 A14 A16 A18 A20 R1 −6.6254E−02 1.9086E−02 −2.6490E−03 — — R2 −9.5365E−02 4.5120E−03 2.2119E−03 — — R3 −1.0041E−01 −1.2929E−02 7.2641E−03 — — R4 −2.5260E−01 1.1125E−01 −2.8530E−02 — — R5 4.5766E−01 −3.2528E−01 9.0532E−02 — — R6 4.1918E−01 −2.6100E−01 6.5242E−02 — — R7 3.3448E−01 −1.6448E−01 3.2738E−02 — — R8 −7.9351E−03 5.9298E−03 −1.2163E−03 — — R9 −2.2877E−02 6.6684E−03 4.3169E−04 −3.9579E−04 3.2796E−05 R10 1.0858E−02 −3.0671E−03 5.1467E−04 −4.9426E−05 2.1096E−06 R11 −4.5055E−03 7.1936E−04 −8.7643E−05 7.1648E−06 −2.7841E−07 R12 −7.9072E−04 −1.7779E−05 1.3217E−05 −1.2153E−06 3.6925E−08

As shown in Table 7, the third embodiment satisfies the various conditions.

FIG. 11 and FIG. 12 show the longitudinal aberration and lateral color schematic diagrams after light with a wavelength of 486 nm, 588 nm and 656 nm passes the camera optical lens in the third embodiment. FIG. 13 shows the field curvature and distortion schematic diagrams after light with a wavelength of 588 nm passes the camera optical lens in the third embodiment. As shown in FIG. 11 to FIG. 13, in this embodiment, the optical length TTL of the camera optical lens is 4.925 mm, the F value Fno is 1.82, it has an excellent optical characteristics with miniaturization and high light flux (Fno).

Table 7 shows the various values of the embodiments 1, 2, 3, and the values corresponding with the parameters which satisfies the various conditions. In addition, the units of the various values shown in table 5 are 2ω (°)

f (mm)

f1 (mm)

f2 (mm)

f3 (mm)

f4 (mm)

f5 (mm)

f6 (mm) TTL (mm)

LB (mm)

IH (mm).

TABLE 7 Embodiment 1 Embodiment 2 Embodiment 3 f1/f 1.043 1.056 1.076 (R1 + R2)/(R1 − R2) −2.188 −2.017 −2.300 (R7 + R8)/(R7 − R8) 11.551 13.700 15.799 f2/f4 0.152 0.154 0.157 R11/f 2.344 2.400 2.450 Fno 1.82 1.82 1.82 2ω 74.7 75.4 74.6 f 4.326 4.179 4.262 f1 4.513 4.413 4.585 f2 −8.396 −9.792 −9.773 f3 8.758 10.026 9.445 f4 −55.061 −63.578 −62.163 f5 4.745 5.063 4.927 f6 −3.069 −3.111 −3.082 TTL 4.942 4.870 4.925 LB 1.042 1.027 1.037 IH 3.300 3.300 3.300

It is to be understood, however, that even though numerous characteristics and advantages of the present exemplary embodiments have been set forth in the foregoing description, together with details of the structures and functions of the embodiments, the disclosure is illustrative only, and changes may be made in detail, especially in matters of shape, size, and arrangement of parts within the principles of the invention to the full extent indicated by the broad general meaning of the terms where the appended claims are expressed. 

What is claimed is:
 1. A camera optical lens comprising, from an object side to an image side in sequence: a first lens having a positive refractive power, a second lens having a negative refractive power, a third lens having a positive refractive power, a fourth lens having a negative refractive power, a fifth lens having a positive refractive power, and a sixth lens having a negative refractive power; wherein the camera optical lens further satisfies the following conditions: 1.00≤f1/f≤1.10; −2.40≤(R1+R2)/(R1−R2)≤−1.90; 11.40≤(R7+R8)/(R7−R8)≤16.00; where f: the focal length of the camera optical lens; f1: the focal length of the first lens; R1: the curvature radius of object side surface of the first lens; R2: the curvature radius of image side surface of the first lens; R7: the curvature radius of the object side surface of the fourth lens; R8: the curvature radius of the image side surface of the fourth lens.
 2. The camera optical lens as described in claim 1, wherein the camera optical lens further satisfies the following conditions: 0.15≤f2/f4≤0.16; where f2: the focal length of the second lens; f4: the focal length of the fourth lens.
 3. The camera optical lens as described in claim 1, wherein the camera optical lens further satisfies the following conditions: 2.30≤R11/f≤2.50; where f: the focal length of the camera optical lens; R11: the curvature radius of object side surface of the sixth lens. 